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混联Ⅱ型惯容非线性能量阱的动力学特性研究

吴子英 朱荣贤 姜东贵 晁国强 张禹轩

吴子英, 朱荣贤, 姜东贵, 晁国强, 张禹轩. 混联Ⅱ型惯容非线性能量阱的动力学特性研究[J]. 应用数学和力学, 2024, 45(7): 907-921. doi: 10.21656/1000-0887.440350
引用本文: 吴子英, 朱荣贤, 姜东贵, 晁国强, 张禹轩. 混联Ⅱ型惯容非线性能量阱的动力学特性研究[J]. 应用数学和力学, 2024, 45(7): 907-921. doi: 10.21656/1000-0887.440350
WU Ziying, ZHU Rongxian, JANG Donggui, CHAO Guoqiang, ZHANG Yuxuan. Research on Dynamic Characteristics of Serial-Parallel-Ⅱ Inerter Nonlinear Energy Sink[J]. Applied Mathematics and Mechanics, 2024, 45(7): 907-921. doi: 10.21656/1000-0887.440350
Citation: WU Ziying, ZHU Rongxian, JANG Donggui, CHAO Guoqiang, ZHANG Yuxuan. Research on Dynamic Characteristics of Serial-Parallel-Ⅱ Inerter Nonlinear Energy Sink[J]. Applied Mathematics and Mechanics, 2024, 45(7): 907-921. doi: 10.21656/1000-0887.440350

混联Ⅱ型惯容非线性能量阱的动力学特性研究

doi: 10.21656/1000-0887.440350
基金项目: 

国家自然科学基金 11572243

详细信息
    通讯作者:

    吴子英(1975—),男,副教授,博士(通讯作者. E-mail: ziyingwu@163.com)

  • 中图分类号: O322;TP113

Research on Dynamic Characteristics of Serial-Parallel-Ⅱ Inerter Nonlinear Energy Sink

  • 摘要: 分别使用非线性恢复力、非线性阻尼替代惯容减振系统中的线性恢复力、线性阻尼,并考虑摩擦力的影响,提出了混联Ⅱ型惯容非线性能量阱. 建立了主系统的动力学方程,利用谐波平衡法求解系统在简谐激励下的幅频响应曲线. 采用弧长算法和数值法相结合的方法研究了系统的惯质比、非线性阻尼、非线性刚度和摩擦力单个参数对其减振性能的影响. 发现非线性刚度和非线性阻尼数值的增大会使峰值先减小后增大,不同的是,前者幅频响应曲线逐渐向右上方向弯曲,后者产生峰值的位置向低频段转移. 分析了惯质比、非线性阻尼、非线性刚度3种参数两两组合下对系统减振效果的影响. 研究表明,在激励幅值为0.005 m时,惯质比和阻尼同时变化减振效果最好:当ε=0.1时,系统主结构位移峰值的最小值约为0.01 m;而在参数ε=0.001时,整体取值范围内其最大值约为0.061 m;当惯质比取得最佳值0.1时,非线性阻尼和非线性刚度κ21的取值范围变大. 在摩擦力的作用下,系统的最大幅值都有不同程度的增加. 上述研究可为振动系统减振的研究提供参考.
  • 图  1  新型混联Ⅱ型惯容NES力学模型

    Figure  1.  Mechanical modeling of a new serial-parallel-Ⅱ inerter NES

    图  2  滚珠丝杠惯容器的工作原理图

    Figure  2.  The ball screw inerter working principle diagram

    图  3  单自由度主系统的力学模型

    Figure  3.  Mechanical modeling of a 1-DOF primary system

    图  4  弧长算法求解示意图

    Figure  4.  Schematic diagram of the arc-length algorithm solution

    图  5  系统幅频响应曲线对比(ε=0.1, A=0.005 m)

    Figure  5.  Comparison of amplitude-frequency response curves of the system(ε=0.1, A=0.005 m)

    图  6  系统幅频响应曲线对比(ε=1, κ22=120)

    Figure  6.  Comparison of amplitude-frequency response curves of the system(ε=1, κ22=120)

    图  7  3种减振系统的力学模型

    Figure  7.  Mechanical models of 3 vibration reduction systems

    图  8  不同减振系统和激励幅值下主结构的幅频响应曲线(ε=0.1)

     为了解释图中的颜色,读者可以参考本文的电子网页版本,后同.

    Figure  8.  The amplitude-frequency response curves of the main structure under different vibration reduction systems and excitation amplitudes(ε=0.1)

    图  9  NES的质量比与减振率的关系曲线

    Figure  9.  Relation curves between the mass ratio of NES and the vibration reduction rate

    图  10  不同刚度比κ21下的系统最大幅值(ε=0.1, A=0.005 m)

    Figure  10.  Maximum amplitude of the system for different stiffness ratios κ21 (ε=0.1, A=0.005 m)

    图  11  不同刚度比κ22下的系统幅频响应曲线(ε=1, A=0.005 m)

    Figure  11.  Amplitude-frequency response curve of the system with different stiffness ratio κ22 (ε=1, A=0.005 m)

    图  12  不同阻尼下的系统幅频响应曲线(ε=1, A=0.005 m)

    Figure  12.  Amplitude-frequency response curve of the system under different damping (ε=1, A=0.005 m)

    图  13  摩擦力对主系统的非线性特性的影响(ε=0.1, A=0.005 m)

    Figure  13.  The influence of friction on the nonlinear characteristics of the primary system (ε=0.1, A=0.005 m)

    图  14  摩擦力下的系统幅频响应曲线(ε=0.1, A=0.005 m)

    Figure  14.  Amplitude-frequency response curve of the system under friction force(ε=0.1, A=0.005 m)

    图  15  刚度和阻尼同时变化对主结构频响曲线峰值的影响

    Figure  15.  Influence of simultaneous stiffness and damping changes on the peak value of the frequency response curve of the main structure

    图  16  刚度和惯质比同时变化对主结构频响曲线峰值的影响

    Figure  16.  Influence of simultaneous stiffness and inertia ratio changes on the peak of the frequency response curve of the main structure

    图  17  惯质比和阻尼同时变化对主结构频响曲线峰值的影响

    Figure  17.  Influence of simultaneous inertia ratio and damping changes on the peak of the frequency response curve of the main structure

    表  1  混联Ⅱ型惯容NES系统的仿真参数

    Table  1.   Simulation parameters of the serial-parallel-Ⅱ inerter NES system

    symbol value
    main structural mass m1/kg 3.3
    inerter parameter b/kg 0.33
    main structure damping c1/(N·s·m-1) 1.4
    linear stiffness k1/(N/m) 2 814
    linear coefficient of nonlinear damping c21/(N·s·m-1) 5
    nonlinear coefficient of nonlinear damping c22/(N·s3·m-3) 5
    linear coefficient of nonlinear stiffness k21/(N/m) 4 814
    nonlinear coefficient of nonlinear stiffness k22/(N/m3) 199 980
    excitation amplitude A/m 0.005
    natural frequency ω1/(rad/s) 29.2
    inertia ratio ε 0.1
    下载: 导出CSV

    表  2  3种减振系统减振效果的对比

    Table  2.   Comparison of vibration reduction effects of 3 vibration reduction systems

    excitation amplitude A/m system name value
    T-NES SP-Ⅱ-Ⅰ I-NES
    inertia ratio εI=0.1 εI=0.1
    mass ratio εm=0.1 εb=0.001 εb=0.001
    0.002 5 Ai/m 0.021 9 0.033 0 0.025 2
    Ri/% 87.2 80.71 85.27
    0.005 Ai/m 0.230 1 0.066 0 0.038 8
    Ri/% 40.63 80.70 88.66
    0.001 Ai/m 0.574 6 0.132 1 0.056 6
    Ri/% 15.61 80.60 91.69
    下载: 导出CSV
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  • 收稿日期:  2023-12-08
  • 修回日期:  2024-02-17
  • 刊出日期:  2024-07-01

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